Heavy Neutral Leptons in Gauged U(1)Lμ−LτU(1)_{L_\mu-L_\tau} at Muon Collider

Abstract

Heavy neutral leptons NN are the most appealing candidates to generate the tiny neutrino masses. In this paper, we study the signature of heavy neutral leptons in gauged U(1)Lμ−LτU(1)_{L_\mu-L_\tau} at a muon collider. Charged under the U(1)Lμ−LτU(1)_{L_\mu-L_\tau} symmetry, the heavy neutral leptons can be pair produced via the new gauge boson Z′Z' at muon collider as μ+μ−→Z′∗→NN\mu^+\mu^-\to Z^{\prime *}\to NN and μ+μ−→Z′(∗)γ→NNγ\mu^+\mu^-\to Z^{\prime (*)} \gamma\to NN\gamma. We then perform a detailed analysis on the lepton number violation signature μ+μ−→NN→μ±μ±W∓W∓\mu^+\mu^-\to NN\to \mu^\pm\mu^\pm W^\mp W^\mp and μ+μ−→NNγ→μ±μ±W∓W∓γ\mu^+\mu^-\to NN \gamma\to \mu^\pm\mu^\pm W^\mp W^\mp \gamma at the 3 TeV muon collider, where the hadronic decays of WW boson are treated as fat-jets JJ. These lepton number violation signatures have quite clean backgrounds at the muon collider. Our simulation shows that a wide range of viable parameter space is within the reach of the 3 TeV muon collider. For instance, with new gauge coupling g′=0.6g'=0.6 and an integrated luminosity of 1000 fb−1^{-1}, the μ±μ±JJ\mu^\pm\mu^\pm JJ signal could probe mZ′≲12.5m_{Z'}\lesssim 12.5 TeV. Meanwhile, if the gauge boson mass satisfies 2mN<mZ′<s2 m_N<m_{Z'}<\sqrt{s}, the μ±μ±JJγ\mu^\pm\mu^\pm JJ\gamma signature would be more promising than the μ±μ±JJ\mu^\pm\mu^\pm JJ signature.Comment: 20 pages, 8 figures, 2 table

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